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ArticlePublished 9 Aug 202623 min readBy Kevin Jogin
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When Are Two Twisted Modules Isomorphic?

Twisting K[X] by the automorphism ii+gi produces a simple An-module for every integrable g, and two such twists are isomorphic exactly when the vectors g coincide. This yields an infinite family of pairwise non-isomorphic simple modules over An.

Collection Algebraic D-modulesTopic stream weyl-modulesSource Ch. 5 §2Reading time 27 minPage ID KVS-ENG-MATH-0353

Overview

Twisting takes a left An-module M and an automorphism σ of An and returns a new module Mσ: the same abelian group, with aAn now acting the way σ(a) used to act. The construction is cheap, it preserves simplicity, and An has a very large automorphism group. So it is a factory for producing modules. The question this page settles is whether the factory produces anything genuinely new, and how one tells two of its products apart.

The answer, for the family that matters most, is completely clean. Fix polynomials g1,,gnK[X] satisfying the integrability condition igj=jgi, and let σg be the automorphism with σg(xi)=xi and σg(i)=i+gi. Then K[X]σg is simple, and

K[X]σgK[X]σhg=h.
(5.1)

Different data give non-isomorphic modules, with no exceptions and no coincidences. Coutinho proves the special case gi=xir, r=1,2,3,, which already gives an infinite family of pairwise non-isomorphic simple An-modules; (5.1) upgrades that to a family indexed by all integrable g, which over is uncountable.

Two mechanisms drive the proof, and both are worth carrying away. First, a homomorphism out of a cyclic module is determined by the image of the generator, so an isomorphism question becomes a differential equation for a single polynomial. Second, a nonzero map between simple modules is automatically an isomorphism, so a non-surjective candidate map is a contradiction rather than a partial result. Beyond this family the isomorphism problem is hard: classifying all simple A1-modules is a genuinely difficult piece of ring theory, and twisting sees only a corner of it.

Definition

Throughout, K is a field of characteristic zero, K[X]=K[x1,,xn], and An acts on K[X] in the standard way: xi multiplies, i differentiates. See the polynomial module for that action and its simplicity.

Twist by an automorphismCoutinho, Ch. 5 §2

Let R be a ring, M a left R-module and σ an automorphism of R. The twisted module Mσ has the same underlying abelian group as M, with the action

au=σ(a)u(aR,uM).

Associativity holds because σ is multiplicative: (ab)u=σ(a)σ(b)u=a(bu).

The exponential twists of the polynomial module

Let g=(g1,,gn) with giK[X] and igj=jgi for all i,j. The assignments xixi, ii+gi preserve all the defining relations of An — the integrability condition is exactly [i+gi,j+gj]=0 — and therefore define an endomorphism σg, which is an automorphism with inverse σg. Write Eg=K[X]σg.

If each gi depends only on xi, integrability is automatic; that is the case Coutinho uses.

Twisting a quotientCoutinho (5.2.1)(4)

For a left ideal J of R and an automorphism σ, (R/J)σR/σ1(J). Indeed the map R(R/J)σ sending bb1¯=σ(b)¯ is a surjective homomorphism of left R-modules with kernel {b:σ(b)J}=σ1(J).

The inverse is not decoration

It is σ1(J), not σ(J). The two choices produce genuinely different modules: for σg one gets An/iAn(igi), whereas the wrong version returns An/iAn(i+gi), and by (5.1) those two are not isomorphic unless g=0.

Core Concepts

Twisting is an action of the automorphism group on isomorphism classes

A direct computation gives (Mσ)τ=Mστ and Mid=M, and an isomorphism MN is still an isomorphism MσNσ. So twisting is a right action of Aut(An) on the set of isomorphism classes of An-modules. Consequently

MσMτMστ1M,
(5.2)

and the whole isomorphism problem for twists of a fixed M collapses to the computation of one subgroup: the stabiliser {σ:MσM}.

Inner automorphisms never help

If σ(a)=uau1 for a unit u, then mum is an isomorphism MMσ, so inner automorphisms lie in every stabiliser. For the Weyl algebra this observation is empty: because Bernstein degree is additive, the units of An are the nonzero scalars, so the only inner automorphism is the identity. Every automorphism of An is outer, and none of them is automatically trivial on isomorphism classes. Which of them act trivially has to be decided case by case.

The twist of K[X] is a differential equation

The module Eg=An/iAn(igi) is the D-module of the system if=gif. Its formal solution is the exponential exp(g), which is a genuine function but not a polynomial. Twisting by σg is therefore the algebraic shadow of the gauge transformation fegf: it multiplies solutions by an exponential factor without changing the underlying vector space. The isomorphism question becomes: when do two exponential factors differ by a polynomial factor? The answer, over a polynomial ring, is never — unless they are equal.

Construction and Proof

Isomorphism criterion for exponential twists

Let g,h be integrable vectors of polynomials. Then every An-homomorphism ϕ:EgEh has the form ϕ(p)=pf for a unique fK[X] satisfying (5.4), and conversely. Consequently EgEh if and only if g=h, and EndAn(Eg)=K.

Proof

Step 1: a homomorphism is multiplication by a polynomial. In both modules xi acts by ordinary multiplication, because σg(xi)=xi. The element 1 generates Eg, and for pK[X] we have p1=p. So ϕ is determined by f:=ϕ(1), and ϕ(p)=ϕ(p1)=pf=pf.

Step 2: equivariance for i is equation (5.4). On the one hand i1=i(1)+gi=gi in Eg, so ϕ(i1)=gif. On the other hand if=if+hif in Eh. Equating gives if=(gihi)f. The computation reverses: if f satisfies these equations then ppf is An-linear, since i(pf)=(ip)f+pif+hipf=(ip)f+gipf=ϕ(ip).

Step 3: a nonzero f forces f to be a constant. Both Eg and Eh are simple, being twists of the simple module K[X]. A nonzero homomorphism between simple modules is an isomorphism, so multiplication by f must be surjective onto K[X]. Multiplication by f has image fK[X], which is all of K[X] only if f is a unit of K[X], that is a nonzero scalar.

Step 4: conclude. If fK× then if=0, so (5.4) gives (gihi)f=0 and hence gi=hi for every i, because K[X] is a domain. Conversely g=h gives the identity map. Taking g=h in Steps 1–4 shows every endomorphism is multiplication by a scalar.

A proof by degree, without simplicity

Step 3 can be replaced by a bare degree count, which is how Coutinho argues (5.2.3). Suppose f0 satisfies (5.4) and gihi for some i. If degxif=0 then if=0, so (gihi)f=0 and the domain property gives gi=hi. If degxif1 then degxi(if)=degxif1, while degxi((gihi)f)degxif. The two sides of (5.4) cannot agree. The degree version is what makes the argument survive when one only knows a nonzero map exists.

An infinite family of simple modulesCoutinho (5.2.3)

The modules K[X]σr, r=1,2,3,, where σr(xi)=xi and σr(i)=ixir, are simple and pairwise non-isomorphic. Over K= the larger family {Eg} is uncountable, so An has uncountably many pairwise non-isomorphic simple modules even though it is a simple Noetherian domain.

Key Equations

The presentation of an exponential twist, obtained by applying the twisting-a-quotient proposition to K[X]An/iAni and σg1(i)=igi:

Eg=K[X]σgAn/i=1nAn(igi).
(5.3)

The equation that any homomorphism EgEh must satisfy, where f is the image of the generator:

fxi=(gihi)f(i=1,,n).
(5.4)

Coutinho's family is gi=xir; for σr:=σ(x1r,,xnr) and r<t, equation (5.4) reads

fxi=(xitxir)f,
(5.5)

which has no nonzero polynomial solution, because the left side has strictly smaller degree in xi than the right.

For n=1 the twists are separated by a numerical invariant as well. With the filtration induced by the generator,

dimKΓm=rm+1,d(K[x]σr)=1,e(K[x]σr)=r.
(5.6)

Variable Definitions

K
the ground field, of characteristic zero
An
the n-th Weyl algebra over K, with generators x1,,xn,1,,n
K[X]
the polynomial ring K[x1,,xn], viewed as a left An-module
K[]
the polynomial ring in the i, viewed as An/iAnxi
σ,τ
automorphisms of An
Mσ
the twist of M by σ, with action au=σ(a)u
g=(g1,,gn)
a vector of polynomials with igj=jgi
σg
the automorphism xixi, ii+gi
Eg
the twisted module K[X]σg
the Fourier transform automorphism, xii, ixi

Properties and Behaviour

What twisting preservesCoutinho (5.2.1)

For any ring R, automorphism σ and left R-module M: Mσ is simple if and only if M is; Mσ is a torsion module if and only if M is; and (M/N)σ=Mσ/Nσ for every submodule N. In fact MMσ is an equivalence of the category of left R-modules with itself, so every purely categorical property — length, indecomposability, projectivity, the lattice of submodules, Ext groups — is preserved.

Dimension is a twist invariant; multiplicity is not

Let σ be an automorphism of An and let c be the largest Bernstein degree of σ(x1),,σ(n), so that σ(Bm)Bcm. If M is finitely generated with generators u1,,uk, the filtration Γm=BmU on Mσ satisfies ΓmΓcm, where Γ is the corresponding filtration on M and U is the span of the generators. Hence dimKΓmχΓ(cm), a polynomial in m of degree d(M), giving d(Mσ)d(M); applying the same argument to σ1 gives equality. The multiplicity only obeys the weaker bound e(Mσ)cde(M), and (5.6) shows it is genuinely not invariant: e(K[x])=1 while e(K[x]σr)=r, with c=r, so the bound is sharp.

In particular twisting preserves holonomicity, which is why all the modules Eg are holonomic — a family of holonomic modules as large as the family of integrable g.

The Fourier transform moves K[X]Coutinho (5.2.2)

Let be the automorphism xii, ixi (an automorphism because [xi,j]=δij). Then 1(i)=xi, so K[X]An/iAnxi=K[]. Moreover K[]K[X]: in K[X] the element 1 is nonzero and killed by every i, whereas in K[] the operator 1 acts by multiplication in a domain and so kills nothing nonzero.

Since 2 sends xixi and ii, we get 2(iAni)=iAni and hence K[X]2K[X]. The orbit of [K[X]] under the cyclic group generated by has exactly two elements, [K[X]] and [K[]].

Some automorphisms of An and their effect on the class of K[X].
AutomorphismAction on generatorsK[X]σClass moved?
Translationxixi+ci, iiK[X]no
Scalingxiλxi, iλ1iK[X]no
Shear in xixi+pi(), iiK[X]no
Exponential twist σgxixi, ii+giAn/iAn(igi)yes, unless g=0
Fourier xii, ixiK[]yes
2xixi, iiK[X]no

Examples and Special Cases

The first twist, r=1

For n=1 and g=x the module is A1/A1(+x), whose analytic solution is exp(x2/2). It is simple, holonomic, and has d=e=1, exactly like K[x] — yet it is not isomorphic to K[x], because f=xf has no nonzero polynomial solution. This is the smallest case where the numerical invariants fail and equation (5.4) is needed.

Twists that change nothing

Take gi=0 but σ a translation xixi+ci, ii. Then σ1 fixes each i, so σ1(iAni)=iAni and K[X]σK[X]. Concretely, translation of the variable permutes polynomials without disturbing the flat vector 1. A nontrivial automorphism can therefore lie in the stabiliser: outer does not mean class-moving.

Two twists in two variables

In A2 take g=(x2,x1), which is integrable since 2x2=1=1x1; the corresponding module is A2/(A2(1x2)+A2(2x1)), with solution exp(x1x2). Take h=(0,0), giving K[X]. By (5.1) they are not isomorphic; equation (5.4) here reads 1f=x2f and 2f=x1f, which no nonzero polynomial satisfies.

The vector (x2,x12) is not integrable (2x2=10=1x12), so it defines no automorphism; the corresponding system 1f=x2f, 2f=x12f is inconsistent, and the module A2/(A2(1x2)+A2(2x12)) is not a twist of K[X].

The Dirac module under Fourier transform

The delta module is A1/A1xK[]. Since 1(x)=, its Fourier twist is A1/A1K[x]. Twisting therefore exchanges the two standard simple modules, matching the analytic statement that the Fourier transform of the delta distribution is a constant.

Worked Example

Separating the twists numerically: e(K[x]σr)=r

  1. Step 1 - fix the module and its action

    Take n=1 and M=K[x]σr with σr(x)=x, σr()=xr and r1. The underlying space is K[x]; the action is

    xf=xf,f=fxrf.

    By (5.3), MA1/A1(+xr). Filter M by Γm=Bm1, where Bm is the Bernstein filtration; this is a good filtration because it is generated by the single generator 1.

  2. Step 2 - compute the first pieces for r=2

    Γ0=K. For Γ1: the spanning set of B1 is 1,x,, acting on 1 to give 1, x, and 1=0x2=x2. So Γ1=K1+Kx+Kx2 and dimKΓ1=3.

    For Γ2: B2 adds x2,x,2. We get xΓ1=Kx+Kx2+Kx3 and (x2)=2x+x4, so x4 enters. Collecting, Γ2=K1+Kx+Kx2+Kx3+Kx4 and dimKΓ2=5. The pattern 1,3,5 matches 2m+1.

  3. Step 3 - prove Γm is the space of polynomials of degree at most rm

    Upper bound: multiplying by x raises degree by 1r, and ffxrf raises it by at most r, so Γm lies in the polynomials of degree rm.

    Lower bound, by induction. Suppose Γm contains every polynomial of degree rm. Then Γm+1Γm+xΓm contains everything of degree rm+1, and for 0jrm we have xj=jxj1xr+jΓm+1, whence xr+jΓm+1 for all such j. Those exponents cover r,r+1,,r+rm, so Γm+1 contains everything of degree r(m+1).

    dimKΓm=rm+1(m0).
  4. Step 4 - read off dimension and multiplicity

    The Hilbert polynomial is χ(m)=rm+1, of degree 1. So d(M)=1=n: every Eg is holonomic. The leading coefficient is r, so e(M)=1!r=r.

    Cross-check against the presentation: for 0PA1 of Bernstein degree d one has e(A1/A1P)=d, and +xr has Bernstein degree max(1,r)=r. The two computations agree.

  5. Step 5 - conclude

    Multiplicity is an isomorphism invariant, so K[x]σrK[x]σt would force r=t. This reproves the corollary for n=1 without touching equation (5.5), and it does more: it exhibits an explicit invariant that separates the members of the family.

Result

K[x]σr is holonomic with d=1 and e=r. In particular r=1 gives e=1, the same multiplicity as K[x] itself, so multiplicity alone does not separate K[x]σ1 from K[x] — for that pair one still needs equation (5.4), which gives f=xf and hence no nonzero polynomial solution.

Applications and Industry Use

In a mathematics topic, this section covers downstream use inside mathematics, computing and engineering rather than a manufactured product.

  • Exponential factors and irregular singularities. Twisting by σg is the algebraic form of multiplying solutions by exp(g). In the analytic theory of irregular connections, exactly these exponential factors are the discrete data attached to a singular point, and (5.1) is the algebraic reason they cannot be absorbed by a polynomial change of variable.
  • Supply of test objects. Every construction in the theory — dimension, characteristic variety, inverse and direct images — needs a stock of modules on which to be tested. The family Eg is cheap, explicit, holonomic, and has adjustable multiplicity, which makes it the natural stress test.
  • Fourier methods. Realising the Fourier transform as a twist converts constant-coefficient operators into polynomials and back. This is what makes the module-theoretic proof of results about constant-coefficient equations short, and it is used in the same way in the theory of the Fourier–Laplace transform of D-modules.
  • Counterexample construction. Because the family is uncountable while An is countable when K is, the twists show that the set of isomorphism classes of simple An-modules is strictly larger than any list of finitely presented normal forms one might hope for. See the catalogue of counterexamples.

Computational Notes

Read this as the manufacturing section of the template: how the object is actually built by machine, at what cost, and where the computation stops being decidable.

Deciding An/IAn/J is an isomorphism test between two cyclic presentations, and it reduces to a Hom computation:

HomAn(An/I,An/J){a¯An/J:IaJ}.
  1. Compute Gröbner bases of I and J in the Weyl algebra with respect to a term order refining the Bernstein filtration.
  2. For increasing degree bounds m, solve the linear system over K describing {aBm:IaJ} modulo J.
  3. For holonomic modules the answer stabilises at a computable bound, so the procedure terminates; a nonzero solution a gives a candidate map, and one checks surjectivity and injectivity by comparing multiplicities.
  4. Cheap pre-filter: compute d and e for both modules first. Different multiplicities settle the question immediately and cost far less than the Hom computation.

The Dmodules package in Macaulay2 implements homomorphism and Ext computations between holonomic modules following Tsai and Walther; dmod.lib in Singular and the ore_algebra package in SageMath provide the underlying Gröbner engines. Note that a negative answer from a degree-bounded search is only conclusive once the bound is justified — an unbounded search that finds nothing proves nothing.

Limits of Validity

The clean criterion (5.1) is a statement about one family, not a general solution to the isomorphism problem.

  • It applies to twists of K[X] by automorphisms fixing all the xi. For a general pair σ,τ the reduction (5.2) still holds, but computing the stabiliser of [K[X]] inside Aut(An) is not settled by anything on this page.
  • Characteristic zero is required. In characteristic p the module K[X] is not simple — the subspace spanned by the p-th powers is a submodule — so Step 3 of the proof collapses, and An itself is no longer simple. See the positive characteristic page.
  • Integrability cannot be dropped. If igjjgi then σg is not an endomorphism of An at all, and the module An/iAn(igi) is something else entirely — it can even be zero.
  • The family does not exhaust the simple modules. Classifying simple A1-modules is a hard open-ended problem; Block's 1981 work reduces it to conjugacy classes of certain irreducible elements, and the exponential twists are only one visible slice of it.

What the criterion does not say

It says nothing about isomorphisms of Eg with modules constructed some other way. For instance the localisation K[x][1/x] is holonomic of multiplicity 2 but is not simple, so it is not an Eg; ruling out such coincidences in general requires invariants beyond (d,e), such as the characteristic variety or the lattice of submodules.

Failure Modes and Common Mistakes

Assuming a cyclic presentation is unique

A cyclic module is An/I for many different left ideals I: the ideal depends on the generator chosen. Take M=K[x] over A1. With the generator 1 we get I=A1. With the generator x — which also generates, since M is simple — we get ann(x)=A1(x1)+A12, and this ideal is not principal: if it were A1P, then e(A1/A1P)=degP would have to equal e(K[x])=1, forcing P=ax+b+c, and no such operator annihilates x. So IJ tells you nothing; only similarity of the ideals does.

Sign errors in the twist, and their cost

The two conventions au=σ(a)u and au=σ1(a)u both define modules, and both appear in the literature. Under the first, K[X]σgAn/iAn(igi); under the second, the sign of g flips. By (5.1) the two answers are non-isomorphic modules whenever g0, so this is not a cosmetic ambiguity. State the convention before computing, and check it against the case gi=0.

Reading "simple ring" as "few simple modules"

P0 is a simple ring, so every nonzero module is faithful and the two-sided annihilator carries no information whatsoever about a module. That is the opposite of a classification: it means the cheap invariant is useless, and the family {Eg} shows there are uncountably many isomorphism classes of simple modules to tell apart.

Expecting numerical invariants to be complete

K[x] and K[x]σ1 have the same dimension (1), the same multiplicity (1), the same length (1), and both are simple and holonomic. They are still not isomorphic. Numerical invariants can only ever separate classes, never certify that two modules agree; for that one needs an explicit map, and (5.4) is the equation it must satisfy.

Historical Notes

Twisting by an automorphism is old and general ring theory; its use here follows Dixmier's 1968 study of the algebra A1, which computed automorphisms, classified certain simple modules, and posed the conjecture that every endomorphism of An is an automorphism — see the Dixmier conjecture. The exponential twists appear there in the guise of the modules attached to g.

The isomorphism problem for simple A1-modules was studied seriously in the late 1970s and 1980s. Block's 1981 paper reduced the classification to data attached to irreducible elements of a localisation of A1, and made clear that no finite list of families would do. Stafford's work on right ideals of An supplied the companion fact for cyclic presentations: left ideals are classified only up to similarity, and the similarity classes are already rich for A1.

Coutinho's Primer keeps to the concrete end of this story, proving that the twists K[X]σr are pairwise non-isomorphic by a degree count on one differential equation. The point of the argument, then as now, is that questions about modules over a very large noncommutative ring can be reduced to a single polynomial identity.

Comparison

Behaviour of invariants under twisting by an automorphism σ of An.
InvariantPreserved by twisting?Witness
Simplicityyestwisting is a category equivalence
Lengthyessubmodule lattice is preserved
Being a torsion moduleyesannMσ(u)=σ1(annM(u))
Dimension d(M)yesσ(Bm)Bcm bounds growth both ways
Holonomicityyesimmediate from dimension
Multiplicity e(M)noe(K[x])=1, e(K[x]σr)=r
Characteristic varietynoV(ξ) for K[x], V(x) for K[x]σr, r2
Isomorphism classnoK[X]K[]K[X]

Key Takeaways

Key points

  • Twisting is a right action of Aut(An) on isomorphism classes, so MσMτ if and only if Mστ1M.
  • For a left ideal J, (An/J)σAn/σ1(J) — with the inverse, not σ.
  • The exponential twist Eg=K[X]σg is the D-module of the system if=gif, and EgEh if and only if g=h.
  • The proof reduces the isomorphism question to the equation if=(gihi)f for a single polynomial f, which forces f to be a nonzero scalar.
  • Coutinho (5.2.3) is the special case gi=xir; over the full family is uncountable, so An has uncountably many simple modules.
  • Dimension and holonomicity survive twisting; multiplicity and the characteristic variety do not — e(K[x]σr)=r.
  • Numerical invariants can separate classes but never certify an isomorphism; only an explicit map does that.

FAQs

Why does an isomorphism have to be multiplication by a polynomial?

Because in every Eg the variables xi act by ordinary multiplication, and 1 generates. A homomorphism is determined by the image f of the generator, and K[X]-linearity then forces ppf. Only the i-equivariance carries information, and that is equation (5.4).

Is every Eg really simple?

Yes. K[X] is a simple An-module, and twisting preserves the submodule lattice exactly, so Eg has no proper nonzero submodules either. Simplicity is what makes Step 3 of the proof work: a nonzero map must be onto.

Could two different automorphisms give the same twisted module?

Certainly — translations, scalings and shears in all fix the class of K[X]. The statement (5.1) is only that within the family {σg} distinct parameters give distinct classes. The stabiliser of [K[X]] in the full automorphism group is large.

How do these modules relate to functions?

Eg presents the system if=gif, whose solution is exp(g). Over that solution lives in the module of holomorphic functions, where it spans a one-dimensional solution space. The module is the algebraic object; the exponential is what it is about.

Does the multiplicity always distinguish the twists?

No. For n=1 the twist by σ1 has e=1, the same as K[x], but the two are not isomorphic. Multiplicity is a genuine invariant and often the cheapest one, but it is far from complete.

What breaks in characteristic p?

Simplicity. In characteristic p the polynomials in x1p,,xnp form a proper nonzero submodule of K[X], since i(xip)=0. The twists are then no longer simple, and An itself has a huge centre, so almost none of the argument survives.

Is there an algorithm that decides isomorphism for arbitrary cyclic modules?

For holonomic modules over An there are terminating Hom and Ext algorithms, so isomorphism of two explicitly presented holonomic modules is decidable in principle. For non-holonomic finitely generated modules no such general procedure is available, and the underlying question — similarity of left ideals — is already delicate for A1.

References

  1. S. C. Coutinho, A Primer of Algebraic D-modules, London Mathematical Society Student Texts 33, Cambridge University Press, 1995 — Ch. 5 §2, results (5.2.1), (5.2.2) and (5.2.3).
  2. J. Dixmier, Sur les algèbres de Weyl, Bulletin de la Société Mathématique de France 96 (1968), 209–242 — automorphisms of A1 and its simple modules.
  3. R. E. Block, The irreducible representations of the Lie algebra sl(2) and of the Weyl algebra, Advances in Mathematics 39 (1981), 69–110.
  4. J. T. Stafford, Endomorphisms of right ideals of the Weyl algebra, Transactions of the American Mathematical Society 299 (1987), 623–639.
  5. J. C. McConnell and J. C. Robson, Noncommutative Noetherian Rings, Graduate Studies in Mathematics 30, revised edition, American Mathematical Society, 2001 — Ch. 1 and Ch. 8, for twisting, similarity of ideals and Gelfand–Kirillov dimension.
  6. J.-E. Björk, Rings of Differential Operators, North-Holland, 1979 — Ch. 1, for filtrations and multiplicity.
  7. H. Tsai and U. Walther, Computing homomorphisms between holonomic D-modules, Journal of Symbolic Computation 32 (2001), 597–617 — the algorithms behind the Dmodules package in Macaulay2.
  8. ISO 80000-2:2019, Quantities and units — Part 2: Mathematics, International Organization for Standardization.

AI Suggested Questions

  • Verify directly that σg preserves the relation [i,xj]=δij, and show that integrability is exactly what is needed for [i+gi,j+gj]=0.
  • Compute the characteristic variety of A1/A1(+xr) for r=1,2,3 and explain why the answer changes at r=1.
  • Show that the stabiliser of the class of K[X] contains every automorphism fixing all the i.
  • Determine whether A1/A1(x) and A1/A1(+x) are isomorphic, and give the polynomial equation that decides it.
  • Prove that the units of An are exactly the nonzero scalars, using additivity of Bernstein degree.
  • Compute e(K[x]σg) for g a general polynomial of degree r and compare with the bound e(Mσ)cde(M).
  • Find an integrable g in two variables that is not a gradient of a polynomial when K has characteristic p, and explain what goes wrong.

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